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带电胶体的沉降:原始模型与有效单组分方法

Sedimentation of charged colloids: the primitive model and the effective one-component approach.

作者信息

Torres Aldemar, Cuetos Alejandro, Dijkstra Marjolein, van Roij René

机构信息

Institute for Theoretical Physics, Utrecht University, Leuvenlaan 4, 3584 CE Utrecht, The Netherlands.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2007 Apr;75(4 Pt 1):041405. doi: 10.1103/PhysRevE.75.041405. Epub 2007 Apr 19.

Abstract

Sedimentation-diffusion equilibrium density profiles of suspensions of charge-stabilized colloids are calculated theoretically and by Monte Carlo (MC) simulations, both for a one-component model of colloidal particles interacting through pairwise screened-Coulomb repulsions and for a three-component model of colloids, cations, and anions with unscreened-Coulomb interactions. We focus on a state point for which experimental measurements are available [C. P. Royall, J. Phys.: Condens Matter 17, 2315 (2005)]. Despite the apparently different picture that emerges from the one- and three-component models (repelling colloids pushing each other to high altitude in the former, versus a self-generated electric field that pushes the colloids up in the latter), we find similar colloidal density profiles for both models from theory as well as simulation, thereby suggesting that these pictures represent different viewpoints of the same phenomenon. The sedimentation profiles obtained from an effective one-component model by MC simulations and theory, together with MC simulations of the multicomponent primitive model are consistent among themselves, but differ quantitatively from the results of a theoretical multicomponent description at the Poisson-Boltzmann level. We find that for small and moderate colloid charge the Poisson-Boltzmann theory gives profiles in excellent agreement with the effective one-component theory if a smaller effective charge is used. We attribute this discrepancy to the poor treatment of correlations in the Poisson-Boltzmann theory.

摘要

通过理论计算以及蒙特卡罗(MC)模拟,得出了电荷稳定胶体悬浮液的沉降 - 扩散平衡密度分布,这一过程既针对通过成对屏蔽库仑排斥相互作用的单组分胶体粒子模型,也针对具有未屏蔽库仑相互作用的胶体、阳离子和阴离子的三组分模型。我们关注的是一个有实验测量数据的状态点[C. P. 罗亚尔,《物理:凝聚态物质》17, 2315 (2005)]。尽管单组分和三组分模型呈现出明显不同的情况(在前者中,相互排斥的胶体将彼此推向高处,而在后者中,是自生电场将胶体向上推),但我们从理论以及模拟中发现,这两种模型的胶体密度分布相似,这表明这些情况代表了同一现象的不同视角。通过MC模拟和理论从有效单组分模型获得的沉降分布,与多组分原始模型的MC模拟结果相互一致,但在定量上与泊松 - 玻尔兹曼水平的理论多组分描述结果不同。我们发现,对于小电荷和中等电荷的胶体,如果使用较小的有效电荷,泊松 - 玻尔兹曼理论给出的分布与有效单组分理论非常吻合。我们将这种差异归因于泊松 - 玻尔兹曼理论中对相关性的处理不当。

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